UV solid light source of inorganic powder

ABSTRACT

An inorganic powder uses a UV solid light source, in which an inorganic powder is based on the inorganic powder of n-silicate group II elements, and its ingredients have valence 2 ions, such as Eu +2 , Sm +2 , Yb +2  and Dy +2 , valence 3 ions Ce +3 , Tb +3  and/or Eu +3 . The chemical formula of the components is Me +2   1-x Ln +3   2-y Si 2 O 8 :TR +2   x :TR +3   y . A main structure thereof is a hexagonal crystal structure. When the indium gallium nitride and gallium nitride based allomorphous semiconductor short wave UV light is used under conditions of excitement, the multiple band white light can be obtained.

BACKGROUND OF THE INVENTION

1. Field of the Invention

An inorganic powder uses a UV solid light source. The chemical formula of main component is Me⁺² _(1-x)Ln⁺³ _(2-y)Si₂O₈:TR²⁺ _(x):TR⁺³ _(y). When the indium gallium nitride and gallium nitride-based allomorphous semiconductor short wave UV light is being used under conditions of excitement, multiple band white light can be obtained.

2. Description of Related Art

In recent years, the manufacturing technology of the solid light source has improved continuously. The efficiency of illumination is greatly increased. Since the solid light source may emit nearly monochrome light, and is highly reliable, enjoys longevity, and can be broadly applied, it has been used in many lighting equipment applications. There is a trend of replacing traditional vacuum light bulbs with solid light sources.

A white light source is mixed from multiple colors of light. The white light that can be observed by human eyes contains a mixture of light with at least two or more wavelengths. When human eyes are simultaneously excited by red, blue and green light, or simultaneously excited by the cross compensation light of blue and yellow light, the light is perceived as white light. This principle can be used to generate a solid light source for the white light.

There are main four conventional means of white solid light source generation. The first method uses three solid light sources using InGaAlP, GaN and GaN as material. The electric current passes, under respective control, through the solid light sources and emits red, green and blue light. Then, a lens is used to mix the light emitted to generate white light.

The second method uses two solid light sources with GaN and GaP as materials. The current passing through these solid light sources is also individually controlled to emit blue and yellow-green light to generate white light. Although the efficiency of illumination for the above mentioned two methods may reach 20 lm/W, if one of the different color solid light sources fails, normal white light cannot be obtained. Additionally, the positive bias is different. Thus, many sets of control electric circuits are required. The cost is high. These are many disadvantages of practical applications.

The third method was developed in 1996 by Nichia Chemical of Japan. An indium gallium nitride blue solid light source and a yellow light-emitting yttrium aluminum garnet fluorescent material are used to form a white light source. Although, at the present time, the efficiency of illumination (as high as 15 lm/W) is lower than those the prior two methods, only one solid light source chip set is required. The manufacturing cost is reduced significantly. Furthermore, the formulation and production technology for the fluorescent material is mature, and commercial products are available.

However, methods two and three utilize a color compensation principle to generate white light. The continuity of spectrum wavelength distribution is not as good as sunlight. After the mixture of the colored light, in the visible light spectrum range (400 nm-700 nm), the color is not even. The saturation of color is low. This phenomenon can be ignored by human eyes, because they only perceive white light. However, high precision optical detectors, such as a video camera or camera, perceive the color rendering as low. Errors will be caused during reduction. Thus, the white light sources generated by these methods can only be used for simple lighting applications.

The fourth white light generating method was developed by Sumitomo Electric Industries, Ltd of Japan. It uses ZnSe material as the white solid light. A CdZnSe thin film is first formed on the ZnSe single crystal baseboard. After energizing, the thin film emits blue light. At the same time, a portion of the blue light shines on the baseboard and emits a yellow light. Finally, the blue and yellow light compensate each other and generate white light. This method utilizes only a solid light source crystal. The operation voltage is only 2.7V, lower than the 3.5V required for a GaN solid light source. Additionally, its generation of white light does not require fluorescent material. However, the disadvantages are that the efficiency of illumination is only 8 lm/W, and the service life is only 8000 hours.

In addition to the aforesaid white light generation methods by a solid light source, according to the prior art there is controlled exciting of Y₃Al₅O₁₂, a co-fluorescent material wave spectrum attempt. The additives used to replace Al are Ga or Sc. Alternatively, Lu, Tb, and Sm are used to replace Y to achieve limited results. However, these fluorescent material radiation light spectrum are normally located in the green-yellow zone of visible light. It cannot integrate the design of solid light source and the soft white light generated by white lamp with equivalent color temperature of T=2800 K-3500 K.

In the current art method announced by J. K. Park, the white solid light source uses Ga—N as a base, and its cold light properties. (“White Light-emitting Diodes of Ga—N-Based Sr₂SiO₄:Eu and the Luminescent. Properties” J. Electrochem. Solid State Lett., vol 5 {2002} p. H11). The chemical composition used is silicate inorganic powder based on strontium compounds and with the chemical formula as Sr_(2-x)Eu⁺² _(x)SiO₄. The principle of illumination of inorganic powders is related to the transfer radiation of Eu⁺² replacement of Sr⁺² ions at the crystal sieve anode nodes. The limited utilization of n-silicate inorganic powder production of standard blue light In—Ga—N allomorphous in a white solid light source is that the short wave wavelength used for self-excitement is around λ≦420 nm, where λ=395 nm, λ=405 nm, and λ=380 nm are used.

Although after the aforesaid n-silicate inorganic powder Sr_(2-x)Eu⁺² _(x)SiO₄ is excited by the UV light, the radiation light spectrum is yellow-green, and cold color-adjusted white light can be obtained. Compared to the production equipment of present art used yttrium aluminum garnet fluorescent material, it has much higher Rendering index. It offers the main advantages of the n-silicate inorganic powder solid light source. However, obtaining this advantage can only be achieved when double portions of inorganic powder mixing agents are used in the solid light source.

In addition to the above-mentioned disadvantages that double portions of inorganic powder mixing agents must be used, the strontium europium based n-silicate material has a very low efficiency. When the angles used for the produced white light diodes Sr_(2-x)Eu⁺² _(x)SiO₄ are between 30° and 120°, the light intensity is J=0.1-0.3 candlelight. At the same time, the temperatures of this diode should not exceed 80-90° C. That is, when a solid light source is heated to these values, the light brightness is reduced by half. In addition, the temperatures used in the generation process of the inorganic powder are T=1100-1200° C. This is not sufficient to combine the quantum effect of the inorganic powders. During the synthesizing of various known silicate inorganic powder, the vitrification of products is easily occurs. This forces the grinding of the vitrified inorganic powder and leads to lower quantum effect.

For the present art that uses UV light as solid light source chips, such as U.S. Pat. No. 6,765,237 “White light-emitting device based on UV solid light source and phosphor blend”, a fluorescent body is provided that is the combination of two chemical components, to achieve the UV light excited white light solid light source.

SUMMARY OF THE INVENTION

This invention relates to a type of UV solid light source's inorganic powder. The components of the inorganic powder include valence 2 ions, such as Eu⁺², Sm⁺², Yb⁺² and Dy⁺², valence 3 ions. Ce⁺³, Tb⁺³, and Eu⁺³. The chemical formula of the component is Me⁺² _(1-x)Ln⁺³ _(2-y)Si₂O₈:TR⁺² _(x):TR⁺³ _(y). In one embodiment, the element is Me⁺²=(among Mg⁺², Ca⁺², Sr⁺², Ba⁺², at least one or more); TR⁺²=(among Sm⁺², Yb⁺², Eu⁺², Dy⁺², at least one or more); TR⁺³=(among Tb⁺³, Ce⁺³, Eu⁺³, Dy⁺³, at least one or more); and Ln⁺³=(among Y⁺³, La⁺³, Gd⁺³, Sc⁺³, Lu⁺³, at least one or more).

The aforesaid structure is mainly a hexagonal crystal structure, ensuring that when the component utilizes indium gallium nitride and gallium nitride based allomorphous semiconductor short wave UV light under conditions of excitement, the multiple band white light can be obtained.

However, the component forms a circulation system for the cation sub lattice. The concentration of each element is: 0≧Mg≦0.2; 0.4≦Ca≦0.8; 0.2≦Sr≦0.4; and 0.2≦Ba≦0.4. The concentration relationship formula is Σ(Me⁺²+TR⁺²)=1.

BRIEF DESCRIPTION OF THE DRAWINGS

No drawings are included with the description of the preferred embodiments.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

This invention utilizes UV light to excited a white solid light source.

The novel combination of the inorganic powder for a UV solid light source is based on the n-silicate II group elements inorganic powder to overcome the defects found in the present art.

A catalyst fluorescent material is proposed. It includes valence 2 ions, such as Eu⁺², Sm⁺², Yb⁺² and Dy⁺²; and valence 3 ions Ce⁺³, Tb⁺³, Eu⁺³, and Dy⁺³.

A stable and standard equipment that can be repeatedly used for the inorganic powder synthesis process is developed.

A new inorganic powder for a short wave solid light source is produced, passing materials to excite the UV light, violet and blue light zones of the visible light, and expand the light spectrum.

For short wave ultra violet and blue solid light source, the n-silicate II and III subgroup based inorganic powders can be used. The chemical formula of the components has the following characteristics: Me⁺² _(1-x)Ln⁺³ _(2-y)Si₂O₈:TR⁺² _(x):TR⁺³ _(y) where Me⁺²=(among Mg⁺², Ca⁺², Sr⁺², Ba⁺², at least one or more); TR⁺²=(among Sm⁺², Yb⁺², Eu⁺², Dy⁺², at least one or more); TR⁺³=(among Tb⁺³, Ce⁺³, Eu⁺³, Dy⁺³, at least one or more); Ln⁺³=(among Y⁺³, La⁺³, Gd⁺³, Sc⁺³, Lu⁺³, at least one or more). The chemical normality index ratio relationships are x=0.000-0.2, y=0.000-0.1. The main crystal lattice is hexagonal crystal structure, which ensures that the fluorescent material can receive the multiple band light radiation coming from the allomorphous semiconductor short wave light.

The aforesaid materials may be called a two dimensional n-silicate with double catalyst. The crystal lattice has two different valence cation fields. Valence two cations, such as Ca, Sr, and Ba form fields with valence values as K1=6 or K1=8. Only after entering Mg⁺² ion into the cation sub lattice, the valence values may then be lowered to K1=4. From another angle, when valence two fields are replaced by large particle Ba⁺² ions, and the valence values may be increased to K1=10 or K1=12. For rare earth elements, such as Y or Gd field, the valence values are lower, such as K2=6 or K2=8. For small particle Lu⁺³ ions, radius r_(Lu)=0.85 A, the reserved valence value is K2=6. When large scale La⁺³ ions are used, the valence values are increased to K2=8 or K2=10.

For the two dimensional n-silicate crystal matrix, the valence value difference for the two cation fields changes as the internal electric fields that affect the layout of catalyst ions inside the lattice nodes. The first and second nodes of the two dimensional n-silicate's crystal lattice are surrounded by oxygen ions. The valence value is lower, K0=4 inside the crystal lattice the SiO₄ tetrahedron on the edge possesses island properties; i.e. they are not in contact with a top or edge. Large-scale silicone oxide tetrahedron is suitable for absorbing the initial exciting energy. Thus, for two dimensional-n-silicate based inorganic powder, not only direct excitement, due to direct transfer of quantum energy toward catalytic ions, is possible, but also the absorption of lattices.

This invention thus describes a series of chemicals: CaLa₂Si₂O₈—CaCl₂Si₂O₈—CaY₂Si₂O₈.

It is determined that these chemicals are completely soluble in cerium components of product solid phase matrix. This is one of the main advantages for recommending n-2-silicate based phase against single phase and n-silicate. Single phase and n-silicate based inorganic powder cannot form a continuous band of catalyst cation (Ce, Nd, Eu) solid solutions, with the same low crystal capacity. That is, the catalyst dissolves, very little within the inorganic powder base materials lattice. The low values of this parameter block the inorganic powder quantity effect from reaching higher values and, normally, with the side effect of lower brightness.

The aforesaid solid state solution is formed through different valence 3 rare earth quantum rare earth cations. It is not the only possible catalyst compounds produced by n-2-silicate. The second type possible is rare earth elements valence 2 ions entering into second tier element cation fields. In the cation sub lattice field Ca⁺², Sr⁺² or Ba⁺² ion locations may be replaced by catalyst ions. Under these conditions, their oxidation levels are +2. These types of valence 2 ions include these ions such as Eu⁺², Sm⁺², Yb⁺², Dy⁺². As when using valence 2 rare earth element ions to replace Ca⁺² ions, in the crystal lattice, these catalytic ions may enter Mn⁺², Sn⁺², and Pb⁺². They belongs typical chemical d-elements. Inside the lattice, the existence of these ions may acquire other wave sections in the light spectrum, such as blue, green, and red, visible light sub-waves.

The above-formed similar multiple band lighting waveforms are very important advantages for the n-2-silicate based inorganic powder families. In practice, in the similar materials, all the known catalyst ions are very active. Table 1 lists the known lighting systems' crystal matrix physical and chemical parameters comparison. It shows that even a small crystal lattice to n-2-silicate ratio may promote the increase of lighting performance. TABLE 1 Compounds No Parameter Me₂SiO₄ Me⁺² ₃Si₃O₁₂ Me⁺² ₁Ln₂Si₂O₈ 1 Crystal system hexahedron Three hexagonal dimension 2 Space group Pnam Ja3d P62m 3 Crystal lattice unit 12 atom 20 atom 14-28 atom volume 4 Solubility of Ln⁺³ Very −10% Average 40% in compounds limited 5 Solubility of Ln⁺² −5% −10% Average 25% in compounds

The distance between the n-2-calcium silicate and lanthanum is 20-25% smaller than the distance between hexagonal n-silicate and cubic silicates. The reduction of distances between ions not only increase the ladder slope inside the crystal field, but also lowers symmetry. These two physical processes will broaden the catalyst light wave spectrum of catalyst inside the n-2-silicate matrix. The wider wave spectrum normally lowers the Lumen value equivalent light. If the standard value is L=380 Lumen/watt, the half span light spectrum spectrum curve is λ_(0.5)=125 nm. Then, for the wider wave spectrum's broadband emission body, this value will be lowered to L=280 Lumen/watt. Then, broad band illumination at the same time will promote, in practice, the duplication of all colors in the full light spectrum range. The last situation indicates that for broadband emitters, the rendering coefficient, Ra, may be increased. Under standard inorganic powder conditions, this coefficient is 62. When excited by UV light, this coefficient is 87.

The advantages of inorganic powder developed in this invention are displayed in the components of the materials. The differences in the materials lie in the formation of the cation sub lattice circulation system. The concentrations of each element are: 0.0≦Mg≦0.2; 0.4≦Ca≦0.8; 0.2≦Sr≦0.4; 0.2≦Ba≦0.4 where the concentration value is: Σ(Me⁺²+TR⁺²)=1. When the rare earth ion contents at the second cation node are: 0.5≦Y≦1.6; 0.1≦La≦0.4; 0.2≦Gd≦0.4; 0.1≦Sc≦0.2; 0.1≦Lu≦0.2

the aforesaid inorganic powder configuration principle is as follows. In the first cation node are all the known IIA family ions, such as Mg⁺², Ca⁺², Sr⁺², and Ba⁺². Apparently, the last 3 ions mentioned before, that is Ca⁺², Sr⁺², and Ba⁺² are compatible. The fourth cation, that is Mg⁺², may exist in a minor amount in the ion components, until gone.

However, three of the four main valence 2 ions are required to produce the inorganic powder. Under these conditions, there are breaks of inorganic powder matrix crystal lattices (volume increase). This increases the solubilities of the 2 valence catalyst ions, such as Sm⁺², Yb⁺², Eu⁺², and Dy⁺². The differences between these valence 2 ions and subgroup Ba⁺² cation are the radiation gram calorie (energy level). This determines the lighting ability and lighting spectrum of the inorganic powder.

The principle of several rare earth elements coexisting inside the lattice cation nodes has been used in this invention for the filing of the inorganic powder ingredient rare earth element (Number 2) node. Within two cation fields, all the five rare earth elements Ln exist that are not equipped with lighting energy (level) within the range of visible light. The inorganic powder components used are Y⁺³, La⁺³, Gd⁺³, Sc⁺³ and Lu⁺³. Among them, the contents of Y⁺³ are 0.5≦Y≦1.6 atomic weight. Among them, La content is between 0.1≦La≦0.4 atomic weight. Thus, it has to be pointed out that the rare earth element ions Y+La belong to two different sub-groups. They are the heavy sub-group and light sub-group, respectively.

To ensure that the group in the second cation node maintains the stability of the unusual combination of these ions, additional ions are added. They are gadolinium ion 0.2≦Gd≦0.4, lutetium ion 0.1≦Lu≦0.2 and scandium ion 0.1≦Sc≦0.2. The inorganic powder base material's crystal lattice will then reach stability at this time. Even at the second field of the lattice, some of the rare earth element ions are replaced by Tb⁺³, Ce⁺³, Eu⁺³, and Dy⁺³ series catalytic rare earth ions. Within the catalyst ions, such as Ce⁺³ and Dy⁺³, exist two different rare earth element sub group. Thus, the five 5 Ln ions can be formed, and, at the same time, the second cation node may be lowered after the introduction of large particle Ce⁺³ ions, and crushed with inorganic powder particles to produce mechanical strength for the lattice.

Adding La⁺³ ion into the ingredients of cation node will increase the chemical parameters of the crystal lattice. At this time, the small particles of lutetium ion Lu⁺³, located at the second part of the lattice crystal node, counter reacts with the lattice dimensions. Through the lowering of the crystal lattice parameters, the static electricity of the inside field increases. This phenomenon, together with the Ce⁺³, Eu⁺³, Tb⁺³, and Dy⁺³ base materials' inorganic powders, leads to the increase of the catalyst ion radiation shift strength. With the increase of the catalyst ion radiation shift strength, the light brightness of the inorganic powder inside the semi-conductor solid light source will increase.

The unique and beneficial properties of this inorganic powder shows in the ingredients of the inorganic powder. The characteristics are the main rare earth element Ln⁺³ and partial replacement of 3 valence catalyst concentration values are equal to Σ(Ln³⁺+TR⁺³)=2 atomic weight. Under these conditions, the individual concentration of the valence 3 catalyst ions of Ce⁺³, Eu⁺³, Tb⁺³; Dy⁺³ groups are between 0.001≦TR≦0.2 atomic weight. This guarantees that the excited Tb⁺³ rare earth element ion node's light spectrum is λ=545±10 nm. When the Ce⁺³ ion is excited, green-yellow light is obtained. The light spectrum is between 525 nm and 575 nm. After adding Eu⁺³ and Dy⁺³ ions to the rare earth element node, the main light spectrum is located in the yellow-orange zones of visible light.

The embodiments of this invention use UV radiation wave lengths of λ<430 nm the solid light source excited inorganic powder light spectrum. The type of ingredients is (Ca, Sr, Ba)(Y, La, Gd, Lu, Sc)₂Si₂O₈. Among them, the Ce⁺³ ion light emission towards broad band zone wavelengths are λ=500 to 720 nm. They include the green, yellow, orange and red color zones of the visible light. The Tb⁺³ ion light spectrum covers Ce⁺³ ion light spectrum. The highest wavelengths in the light spectrum are green light and yellow light with sub-energy band perimeter wavelength as λ=545±10 nm. Using the europium ion to excite, the light emmission will appear in the orange light spectrum zone λ=610-625 nm. The excited catalyst ion Dy⁺³ is a narrow band spectrum. The highest spectrum value is λ=576 nm.

From the above information, it can be determined that inorganic powder radiations may be broadband and narrow band. The radiation movement changes at the same time. For example, Ce⁺³ ion has very short radiation, equals to τ≦100 ns. The properties of Tb⁺³ and Eu⁺³ inorganic powder are that the residual light's average time is between 1 to 5 ms.

The aforesaid high light spectrum kinetic properties are shown in their ingredient properties. The material absorption spectrum, when using europium ion (Eu⁺²) and/or samarium ion (Sm⁺²) and/or ytterbium ion to catalyze the inorganic powder, tends toward blue and sky blue sub-energy bands of the visible spectrum. At this time, the aforesaid ion radiation wavelengths are at the green-sky blue subenergy band, and the half span of the radiation band is λ_(0.5)=40-80 nm.

The Eu⁺², Sm⁺², and Yb⁺² series valence 2 rare earth element ion excites the first cation node results that inorganic powder particle emits sand color-yellow color. This is related to the special energy conditions; that is, the electric shift band between O⁻² and TR⁺ ion, inside the inorganic powder lattice. This strong energy band presents strong absorption wavelength for short wave between 400 nm and 480 nm to color the inorganic powder. Normally, through adding Eu⁺², Sm⁺² and even Yb⁺² to the ingredients of inorganic powder, the surface color of the inorganic powder is increased.

The use of Eu⁺² catalyzed n-silicate inorganic powder light spectrum has special properties (wavelengths between 480 and 530 nm). Sm⁺² catalyzed inorganic powder wavelength is (540 to 590 nm). Yb⁺² catalyzed inorganic powder wavelength is (420 nm).

After synthesizing the above-mentioned inorganic powder, the particle diameters are averaging 0.6-12 micrometers. After grinding to particle diameters below 2 to 3 micrometers, the performance will not be lost.

In the embodiment of this invention, to form light emission coating on the solid light source, the prepared polymer mixing materials using a melting glue as a base material are used. The mixing materials include at least a melting glue, epoxy, or silicone (step 1). Afterwards, when the suspended material concentration is the lowest, the inorganic powder is then coated, layer by layer, onto the surface of the solid light source allomorphous (step 2). The thickness of each layer is 30-40 micrometers. For inorganic powder with a higher concentration of suspended material the thickness may be 60-70 micrometers, as a single layer, for coating on the surface of the allomorphous solid light source.

Then, the amino allomorphous coated with inorganic powder is welded into the body of the metal shell. (Step 3). Then, a lens polymer cover is added (Step 4). Between the shell inside surface and the inorganic powder polymer coating layer, two silicone oxide melting glues and polymer mixing materials are added. (Step 5).

In the aforesaid structure, the voltage supply to the allomorphous electrodes is V_(F)=4V. The current is I_(F)=50 mA. The observed white light color temperature T=4500 K is as strong white light. When the light strength of the diode is at 2Θ_(1/2)=20′, it reaches J=2 candle light. As mentioned above, the novel inorganic powder chemical structure for a UV solid light source is a rare invention. The requirements for industrial applications, innovation and advancement are all met. Thus, this application is submitted in accordance with the law.

The aforesaid embodiments serve as examples, only. They are not intended to limit the scope of this invention. 

1. A type of inorganic powder for a UV solid light source, the construction ingredients' chemical formula is Me⁺² _(1-x)Ln⁺³ _(2-y)Si₂O₈:TR⁺² _(x):TR⁺³ _(y), wherein: Me⁺²=(wherein Mg⁺², Ca⁺², Sr⁺², Ba⁺², at least one or more); TR⁺²=(wherein Sm⁺², Yb⁺², Eu⁺², Dy⁺², at least one or more); TR⁺³=(wherein Tb⁺³, Ce⁺³, Eu⁺³, Dy⁺³, at least one or more); Ln⁺³=(wherein Y⁺³, La⁺³, Gd⁺³, Sc⁺³, Lu⁺³, at least one or more); wherein a major configuration of an allomorphous surface of the solid light source is a hexagonal crystal structure, guaranteeing a solid light source allomorphous short wave, under UV light excitement, obtainment of multiple band white light.
 2. The inorganic powder for a UV solid light source as claimed in claim 1, wherein ingredients form a cation sub lattice circulation system, and a concentration of each element is: 0≦Mg≦0.2; 0.4≦Ca≦0.8; 0.2≦Sr≦0.4; and 0.2≦Ba≦0.4.
 3. The inorganic powder for a UV solid light source as claimed in claim 1, wherein an ingredient concentration relationship is Σ(Me⁺²+TR⁺²)=1.
 4. The inorganic powder for a UV solid light source as claimed in claim 1, wherein contents of rare earth ion in the second cation node are: 0.5≦Y≦1.6; 1≦La≦0.4; 2≦Gd≦0.4; 1≦Sc≦0.2; and 0.1≦Lu≦0.2.
 5. The inorganic powder for a UV solid light source as claimed in claim 1, wherein a rare earth element Ln⁺³ and partially replaced valence 3 catalyst concentration is Σ(Ln⁺³+TR⁺³)=2 atomic weight.
 6. The inorganic powder for a UV solid light source as claimed in claim 1, wherein individual concentrations of the Ce⁺³, Eu⁺³, Tb⁺³, and Dy⁺³ group valence 3 catalyst ions are about 0.001≦TR≦0.2 atomic weight.
 7. The inorganic powder for a UV solid light source as claimed in claim 1, wherein a UV light excited Tb⁺³ rare earth element ion node light spectrum zone is λ=545±10 nm.
 8. The inorganic powder for a UV solid light source as claimed in claim 1, wherein when the UV light excites Ce⁺³ ion, green-yellow light is obtained, and a spectrum wavelength is from about 525 nm to 575 nm.
 9. The inorganic powder for a UV solid light source as claimed in claim 1, wherein after a UV light excited inorganic powder with Eu⁺³ and Dy⁺³ in is added, a main visible light spectrum is in visible light's yellow-orange zone.
 10. The inorganic powder for a UV solid light source as claimed in claim 1, wherein when an inorganic powder material absorption spectrum is catalyzed by europium ion (Eu⁺²) samarium ion (Sm⁺²) ytterbium ion or a combination thereof, an absorption spectrum is in a blue-sky blue energy band, a radiation wavelength is in a green-sky blue sub-energy band of the spectrum and a half span wavelength of the radiation band is between about 40 nm and 80 nm.
 11. The inorganic powder for a UV solid light source as claimed in claim 1, forming the inorganic powder on the solid light source, the production procedure including: preparing a polymer mixing materials, including melting glue, epoxy, silicone, or a combination thereof; coating an allomorphous surface of the solid light source with inorganic powder; welding the inorganic powder with amino allomorphous to a metal shell; install a polymer lens cover; and filling between a shell inside surface and an inorganic powder polymer coating layer with a polymer material.
 12. The inorganic powder for a UV solid light source as claimed in claim 1, wherein the inorganic powder is coated on the allomorphous, layer by layer, when an inorganic powder suspended material concentration is at a minimum.
 13. The inorganic powder for a UV solid light source as claimed in claim 1, wherein an inorganic powder thickness is 30-40 micrometers, and for higher concentration inorganic powder suspended materials, a thickness may be an about 60-70 micrometers single layer coating on the allomorphous semiconductor surface. 